Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 65
The matrix V / dx , dx , corresponds to our operator F and is obviously self - adjoint , since it is symmetric . Our theory corresponds to a continuum of dimensions but is otherwise algebraically the same . The proof of d ) follows the ...
The matrix V / dx , dx , corresponds to our operator F and is obviously self - adjoint , since it is symmetric . Our theory corresponds to a continuum of dimensions but is otherwise algebraically the same . The proof of d ) follows the ...
Page 148
... . The signifi- cance of this is that for large k and low ẞ only pure electrostatic waves are possible . Thus , if we write down the dispersion matrix FXVXE + E = 1лj in a co - ordinate system in which one of 148 M. N. ROSENBLUTH.
... . The signifi- cance of this is that for large k and low ẞ only pure electrostatic waves are possible . Thus , if we write down the dispersion matrix FXVXE + E = 1лj in a co - ordinate system in which one of 148 M. N. ROSENBLUTH.
Page 149
... matrix has the fol- lowing structure : - ( k2 — v2 + ( α11 ) ( α12 ) ( α13 ) ( 3.1 ) ( X21 ) k2 — v2 + ( X22 ) ( X23 ) ( X31 ) ( x32 ) -22 + ( α33 ) / - = 0 , where the quantities ( x ,, ) arise from the plasma currents and are all of ...
... matrix has the fol- lowing structure : - ( k2 — v2 + ( α11 ) ( α12 ) ( α13 ) ( 3.1 ) ( X21 ) k2 — v2 + ( X22 ) ( X23 ) ( X31 ) ( x32 ) -22 + ( α33 ) / - = 0 , where the quantities ( x ,, ) arise from the plasma currents and are all of ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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adiabatic invariant amplitude approximation Boltzmann equation boundary conditions boundary layer calculated cathode coefficient collision components consider constant contraction corresponds courbe critère current density d³k d³v Debye length derived differential equations discharge dispersion relation distribution function eigenvalue electric field electrons and ions electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ KRUSKAL l'axe magnétique limit Liouville function lowest order magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle périodique perturbation Phys plasma oscillations Plasma Physics Poisson's equation potential problem quantities R₁ region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity x₁ zero zero-order Απ